Possible Time Point for Electron Moving in Opposite Direction

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Homework Help Overview

The problem involves an electron moving at a speed of 1 x 10^6 m/s entering a uniform magnetic field of 6 mT, which is perpendicular to its velocity. The question seeks to determine a time point when the electron will move in the opposite direction of its final velocity after entering the magnetic field.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the nature of the magnetic force acting on the electron, noting that it is always perpendicular to the velocity and does not change the speed. There is exploration of the circular path that the electron will take due to this force. Questions arise regarding the calculation of the radius of the orbit and the implications of the angle between the velocity and magnetic field vectors.

Discussion Status

Participants are actively exploring the implications of the magnetic force on the electron's motion, with some providing hints and guidance on visualizing the path and calculating the radius of the orbit. There is recognition of the need to clarify the relationship between the vectors involved and the nature of the circular motion.

Contextual Notes

Participants are considering the constraints of the problem, including the perpendicular nature of the velocity and magnetic field, and the assumptions about the motion of the electron in a magnetic field.

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Homework Statement



An electron with speed of [tex]1o^{6} m/s[/tex] enters a [tex]6mT[/tex]
uniform magnetic field that is perpendicular to the velocity of the electron. What is one possible time point after the electron entered the magnetic field that the electron will move along the opposite direction from its final velocity?

Homework Equations





The Attempt at a Solution



Since the velocity of the electron and the magnetic field are perpendicular,

[tex]F_{B} = qv_{o}B = ma[/tex]

So,

[tex]a = \frac{qv_{o}B}{m}[/tex]

But,

[tex]v_{f} = 0 = v_{o} + at[/tex]

So,

[tex]t = \frac{-m}{qB}[/tex]

Where am I going wrong?
 
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It's extremely important to keep track of the direction of the force. Since the magnetic force is always perpendicular to the velocity, it does not change the speed of the electron. You should try to visualize the path of the electron and rethink the question.
 
It should pull the electron into a circular path, correct ?
 
Bump, still trying to figure this one out, can I get another hint?
 
Yes, it will be a circular path. You know the speed of the electron and can calculate the force. Can you figure out the radius of the orbit?
 
fzero said:
Yes, it will be a circular path. You know the speed of the electron and can calculate the force. Can you figure out the radius of the orbit?

[tex]F_{B} = qv \times B[/tex]

So,

[tex]qv \times B = \frac{mv^{2}}{r}[/tex]

[tex]r = \frac{mv^{2}}{qvBcos\theta}[/tex]

Is theta changing though? Because as the force starts to push the electron down into a circular path the angle between v and B must be different, correct?
 
You're told that [tex]\vec{v}[/tex] and [tex]\vec{B}[/tex] are perpendicular, so you might want to rethink how you computed the cross product. You should probably draw a diagram to see the relative directions of [tex]\vec{v}[/tex], [tex]\vec{B}[/tex] and [tex]\vec{F}[/tex].
 
fzero said:
You're told that [tex]\vec{v}[/tex] and [tex]\vec{B}[/tex] are perpendicular, so you might want to rethink how you computed the cross product. You should probably draw a diagram to see the relative directions of [tex]\vec{v}[/tex], [tex]\vec{B}[/tex] and [tex]\vec{F}[/tex].

Whoops, I thought they would no longer be perpendicular once the electron started moving in a circular path but that's not true.

So, [tex]\theta = 0^{o}[/tex]

Therefore,

[tex]r = \frac{mv^{2}}{qvB} = \frac{mv}{qB}[/tex]
 

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